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Microscopic view about Raoult law and Henry Law x B k x,A A p k x,B B p A B A A A x k p , x A A p p B B x, B x k p B B B x p p x B →0 x B →1 p Solvent molecule Solute molecule

Microscopic view about Raoult law and Henry Law

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p. k x,B. k x,A. Solute molecule. Solvent molecule. A. B. x B. x B →0. x B →1. Microscopic view about Raoult law and Henry Law. Gas A,B y A ,y B. Liquid A, B x A ,X B. Ideal solution. The solvent and solute both follow Raoult Law. Binary system. Scuba diving. - PowerPoint PPT Presentation

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Page 1: Microscopic view about Raoult law and Henry Law

Microscopic view about Raoult law and Henry Law

xB

kx,A

Ap

kx,B

Bp

A B

AAA xkp ,x

AAA xpp

BBx,B xkp

BBB xpp

xB→0 xB →1

p

Solvent molecule

Solute molecule

Page 2: Microscopic view about Raoult law and Henry Law

Ideal solution

Binary system *A A A AP Py P x

LiquidA, BxA,XB

GasA,ByA,yB

The solvent and solute both follow Raoult Law

*B B B BP Py P x

*

*

( ln) ( ) ( , ) ln

( , ) ln

( , ) ln

( ) ln

AA A

A A

A

A

Pys gas T P RT

P

P xT P RT

P

T l RT x

T RT x

( ln) ( ) ( ) lnB B Bs g T RT x

* *A A A By x if P P

* *A A A By x if P P

Page 3: Microscopic view about Raoult law and Henry Law

Vaporizable solutes follow Henry Law

kX,B(kPa)(298K)/H20

H2 N2 O2 CO2 CH4

7.12x106 8.68x106 4.40x106 1.66x106 4.18x106

4 17.9 10 . .kPa kg mol

2

2 4 1

4 1

1

21

7.1 10 . .

2.9 10 .

0.29 .

oO

m

P kPam

k kPa kg mol

mol kg

mmol L

25 , sea level, O℃ 2 in air PO2=21kPa

m BBp k m

Scuba diving

Page 4: Microscopic view about Raoult law and Henry Law

Ideal diluted solution

*p p xp p k x A AA B x,B B

Solvent follow Raoult’s law

)/ln()(),( ppRTTpT AAA

AAA xRTppRTT ln)/ln()(

AA xRTpT ln),(*

Solute follow Henry’s law

)/ln()(),()1( ppRTTpT BBB

BxB xRTpkRTT ln)/ln()(

BB xRTpT ln),(*

P

xA

kA*AP

Chemical potential of B, X=1, follow Henry Law

Page 5: Microscopic view about Raoult law and Henry Law

ln)sln()sln( O22 RT 2x

)/( Ommln)sln()sln( O22 RT

)/( Occln)sln()sln( O22 RT

Chemical potential of reference/standard state :

ln)()sln( OO2 RTg )/( O

, pK xh

)/( OO, pmK mh

)/( OO, pcK ch

ln)()sln( OO2 RTg

ln)()sln( OO2 RTg

Solute in diluted solution

Page 6: Microscopic view about Raoult law and Henry Law

4.5 Colligative properties of diluted solution

B

*

AA

*

A xpppp The solute is not volatile

Freezing-point depression

The decrease of vaporizing pressure

f f BT k m f

*

ff TTT

b b BT k m *

bbb TTT

solute

solvent

The elevation of boiling point

Osmosis: osmotic pressure

Page 7: Microscopic view about Raoult law and Henry Law

Freezing-point depression

(l) (s) Tf* (sln) (s) Tf

1(sln) = 1*(s)

R

TG

RT

Gx mfusmfus )/(

lnOO

1

1(l) + RT ln x1 = 1

(s)

RT ln x1 = –[1(l) – 1

(s) ]

p

mfus

p T

TG

RT

x

)/(1ln

O

1

2

O

RT

HmfusHG

ff

mfus

TTR

Hx

11ln

O

1

f

f

T

T

mfusx

T

dT

R

Hx

*

1

2

O

1 1ln

Page 8: Microscopic view about Raoult law and Henry Law

X2 is small lnx1=ln(1– x2) x2

ff

ff

ff TT

TT

TT

11 Tf should be small, too

f

f

mfus TRT

Hx

2

O

2

mKmH

MRTT f

mfus

ff

O

1

2

1

2

21

2

n

n

nn

n

2

f

f

T

T

111

12 mMMn

Mn

A

Am,fus

2*

ff

)(M

H

TRk

freezing point lowering coefficients

1K mol kg 。

Note: diluted solution, separate pure solid (solvent)

Page 9: Microscopic view about Raoult law and Henry Law

Boiling-point elevation

bb

mvap

TTR

Hx

11ln

O

1

mKmH

MRTT b

mvap

bb

O1

2

A

Am,vap

2*

bb

)(M

H

TRk

b b BT k m *

bbb TTT

(boiling point elevation coefficients ), Unit: kgmolK 1 bk

Page 10: Microscopic view about Raoult law and Henry Law

Osmosis phenomenon and osmosis pressure

( ln)A s* ( )A l

mT

VP

Semipermeable membrane

AA((slnsln)=)=AA((ll) +) + RT RT lnln x xAA <<AA*(*(ll))

P↑, μ ↑

*( ln, , ) ( )A A As x p l

Osmosis pressure

Page 11: Microscopic view about Raoult law and Henry Law

* ( , )A l P

ln(1 )B Bx x

*

*

( ln, , )

( , ) ln

( , ) lnA

A A

A A

P

A

P m

s x P

l P RT x

l P V dP RT x

lnP

m A

P

V dP RT x

( )m BV P P RTx

Osmosis pressure: meaning, measurement and application

B

m

xRT cRT

V

Van’t Hoff equation

gh

20℃ , mB=0.001mol.kg-

1

Δp=0.053Pa;ΔTf=0.002K; π=2400Pa

Page 12: Microscopic view about Raoult law and Henry Law

Colligative properties of diluted solution: Application examples

Mr. Tian Wen-fei Mr. Tian Wen-zhi

Page 13: Microscopic view about Raoult law and Henry Law

4.6 Real solution: activity of solute and solvent

i i i ix a x

*ii i

P

P x Or by Henry Law

ii

i i

P

k x Judged by Raoult law

γcs2

γacetone

By R.L.

Page 14: Microscopic view about Raoult law and Henry Law

Determination of activity of solvent

RT

Va m

1,1ln)4(

(1) p1 = p1* a1

ff

mfus

TTR

Ha

11ln)2(

O

1

bb

mvap

TTR

Ha

11ln)3(

O

1

Page 15: Microscopic view about Raoult law and Henry Law

Example 1: Activity of water in aqueous solution

16025 .fus mH J mol * 273.2

258.2

f

f

T K

T K

* 5 3 1, 1.8 10 .m waterV m mol

P0, Aqueous solution Tf=– 15℃

Question: a(water)=? Osmosis pressure of the solution.

Answer:

ff

mfus

TTR

Ha

11ln

O

11543.0

258

1

273

16025

R

a1=0.857

PaaV

RT

m

751

1,

1012.2108.1

1543.0298314.8ln

Page 16: Microscopic view about Raoult law and Henry Law

Example 2: Acetic acid(A)/benzene(B) solutionxA 0 0.0835 0.2973 0.6604 0.9931 1.000

pA /Pa 1535 3306 5360 7293 7333

pB /Pa 35197 33277 28158 18012 466.6

*

18012 / 315791.507

0.3396B B

BB B B

a P

x P x

18012 / 676230.7845

0.3396B A

BB B A

a P

x k x

P

xA0 1

40000Pa

PA

PB

By R.L

By H.L

*

5360 / 73330.731

0.6604A A

AA A A

a P

x P x

By R.L:

Pa

dx

dpK

B

B

xBxh

B

676230069.0

6.466

lim0

,,

mixG=RT(xA ln aA + xB ln aB)= – 1167J

Page 17: Microscopic view about Raoult law and Henry Law

Homeworks Y:P101:15; P104:17,18 P106: 22 P110:23 A: P190: Exe7.19(b); Problem7.1 P192: application7.23

Term seminar report :

May 21:

May 23:

May 30:

June 04:

June 06:10 min/person